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Topology and Dynamics: Rokhlin Memorial
August 19-25, 1999
Steklov Institute of Mathematics at St. Petersburg
St. Petersburg, Russia

Organizers
N. Netsvetaev, A. Vershik, O. Viro

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An equivariant analog of the Poincare-Hopf theorem
by
Konstantin Feldman
Moscow State University

We introduce a new concept of the index of the zero of the tangent vector field on the smooth manifold. This concept generalizes the usual index of the non-degenerated isolated zero of the smooth tangent vector field. On the basis of this concept we prove an equivariant analog of the classical Poincare-Hopf theorem. As an application of the main result we deduce an exact addition formula for the first-half integer Pontryagin class in complex cobordism.

Let us consider a tangent vector field s on a smooth manifold M. We denote the connected component of the zero set of s as M1. We assume that M1 is a closed compact submanifold of M. There is such a deformation of s in an open neighborhood N(M1) of M1, that the vector field s defines a map:
s|N(M1): \nu(M1) -->
~
\tau
 
(\nu(M1)),
where \nu(M1) is a normal bundle of an inclusion M1 subset M, [(\tau)\tilde](\nu(M1)) a tangent bundle along the fiber. Note that [(\tau)\tilde](\nu(M1)) =~ p*\nu(M1), where p:\nu(M1) --> M1 is a projection. We define the produced bundle map as [p\tilde]:[(\tau)\tilde](\nu(M1)) --> \nu(M1). There is such a vector bundle \zeta that \nu(M1)\oplus\zeta is a trivial vector bundle.

Definition 1. The index of the zero set M1 of the vector field s is an element of \pi0S(M+1). The element is defined by the equivalent class of the following map:
j:SN /\ M+1 = T(\nu(M1)\oplus\zeta)
(
~
p
 
, id)

-->
 
T(\nu(M1)\oplus\zeta) \pi
-->
 
SN.

Let \tau(p) be the transfer map for the fibre bundle (E, F, B, p) with the closed compact smooth fibre F without boundary. We assume that there is a vector field s, tangent to E along the fibre. Let E1, ..., Em be the irreducible components of the zeros of the vector field.

Theorem 1. The stable homotopical equality holds
{\tau(p)}= m
å
j=1 
i*j({Inds(Ej)}{\tau(pj)}),
where \tau(pj) is the transfer map for Ej, ij:Ej --> E is an inclusion.

We fix a cogomology theory h*(·) and assume that all bundles E, E1, ..., Em are h-orientated in addition to the conditions of theorem 1.

Corollary 1. We fix w in h*(E). Suppose that there is an element \Delta in h*(E), which does not divide zero, and the Euler class of the tangent bundle to E along the fibre divides p*(\Delta)w. Then the following decomposition formula for the Gysin map holds
p!(w)= m
å
j=1 
pj! \frac Inds(Ej)i*j(w)e(\nuj),
where e(\nuj) is the Euler class of the normal bundle Ej subset E in h*(·).

Theorem 2. There are such elements \betaij in \OmegaU that for the first half-integer Pontryagin class in complex cobordism the addition formula holds:
p1/2(\xi\oplus\zeta)=u+v+
å
i, j >= 1 
\betaij si-1(u)sj-1(v),
where u=p1/2(\xi), v=p1/2(\zeta), sm are the Landveber-Novikov operations.

[]
V.M.Buchstaber, K.E.Feldman, The index of the equivariant vector field and the addition theorems for the Pontryagin characteristic classes, (to appear in Izv. RAS).

Date received: June 2, 1999


Copyright © 1999 by the author(s). The author(s) of this document and the organizers of the conference have granted their consent to include this abstract in Atlas Conferences Inc. Document # cacy-25.